Morgan Pierre

A SPLITTING METHOD FOR THE CAHN–HILLIARD EQUATION WITH INERTIAL TERM

P. Galenko et al. proposed a Cahn–Hilliard model with inertial term in order to model spinodal decomposition caused by deep supercooling in certain glasses. Here we analyze a finite element space semidiscretization of their model, based on a scheme introduced by C. M. Elliott et al. for the Cahn–Hilliard equation. We prove that the semidiscrete solution converges weakly to the continuous solution as the discretization parameter tends to 0. We obtain optimal a priori error estimates in energy norm and related norms, assuming enough regularity on the solution. We also show that the semidiscrete solution converges to an equilibrium as time goes to infinity and we give a simple finite difference version of the scheme.

Mesh optimization for singular axisymmetric harmonic maps from the disc into the sphere

We describe in a mathematical setting the singular energy minimizing axisymmetric harmonic maps from the unit disc into the unit sphere; then, we use this as a test case to compute optimal meshes in presence of sharp boundary layers. For the well-posedness of the continuous minimizing problem, we introduce a lower semicontinuous extension of the energy with respect to weak convergence in BV, and we prove that the extended minimization problem has a unique singular solution. We then show how a moving finite element method, in which the mesh is an unknown of the discrete minimization problem obtained by finite element discretization, mimics this geometric point of view. Finally, we present numerical computations with boundary layers of zero thickness, and we give numerical evidence of the convergence of the method. This last aspect is proved in another paper.

CONVERGENCE OF EXPONENTIAL ATTRACTORS FOR A TIME SEMI-DISCRETE REACTION-DIFFUSION EQUATION

We consider a time semi-discretization of a generalized Allen–Cahn equation with time-step parameter

CONVERGENCE TO EQUILIBRIUM FOR THE BACKWARD EULER SCHEME AND APPLICATIONS

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STABLE DISCRETIZATIONS OF THE CAHN-HILLIARD-GURTIN EQUATIONS

τ. For every

Stationary solutions to phase field crystal equations

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